|Número de publicación||US4843468 A|
|Tipo de publicación||Concesión|
|Número de solicitud||US 07/072,889|
|Fecha de publicación||27 Jun 1989|
|Fecha de presentación||14 Jul 1987|
|Fecha de prioridad||14 Jul 1986|
|También publicado como||DE3783525D1, DE3783525T2, EP0253608A2, EP0253608A3, EP0253608B1|
|Número de publicación||07072889, 072889, US 4843468 A, US 4843468A, US-A-4843468, US4843468 A, US4843468A|
|Inventores||John O. Drewery|
|Cesionario original||British Broadcasting Corporation|
|Exportar cita||BiBTeX, EndNote, RefMan|
|Citas de patentes (8), Citada por (145), Clasificaciones (10), Eventos legales (7)|
|Enlaces externos: USPTO, Cesión de USPTO, Espacenet|
This invention relates to video scanning systems for use for example in television.
Transmission of images by television is conventionally performed by raster scanning in which a signal is formed by scanning the image in a series of parallel lines, either horizontal or vertical. In broadcast television the scan starts at the top left hand corner and finishes at the bottom right hand corner, the scan lines being horizontal. Moreover, each line is scanned in the same direction so that the scan must return to the beginning of each line in, ideally, an infinitessimally short time. Such an action is known as the flyback.
The scanning in conventional imaging and display devices is by way of a continuously moving electronic beam which is deflected by electric or, usually, magnetic fields. With such devices the beam flyback takes a finite time which is, therefore, an "overhead". The horizontal scanning waveform, which is proportional to the deflecting field, therefore appears as in FIG. 1, the idealised version of which is known as a sawtooth waveform.
Similarly, the vertical scanning waveform needed to ensure the equal spacing of the scan lines is another sawtooth, though of much lower frequency. This has a corresponding flyback, imposing a further "overhead". It should be noted that the continuous nature of the vertical scan imposes a continuous vertical displacement on the scan lines so that they are not strictly horizontal. However, the skew thus imposed is negligible.
The large rate of change of the flyback in the horizontal scan waveform is used to provide the high voltage needed in a conventional CRT display. However, it can cause problems if the line rate is increased to provide scanning for higher definition formats since the flyback time of conventional deflection circuits may become a significant proportion of the line period. For this reason, UK Patent Application No. 2,137,844A has proposed a boustrophedonic scanning format in which lines are alternately scanned in opposite directions. This requires a triangular form for the horizontal scan waveform as shown in FIG. 2 (a). This eliminates the flyback, but the sawtooth of the vertical scan must now be modified to a stepped form as shown in FIG. 2 (b) to ensure that adjacent lines are parallel. It also requires that nonlinearities in the horizontal scan waveform result in a symmetrical function as shown in FIG. 3.
A disadvantage of raster-based scanning is that it is committed to a standard in the form of lines in the picture. This means that once an image scanning standard is chosen the display must adopt the same standard, or convert the incoming signal to its own line standard, which is a complex and costly process. Moreover, any curtailment in the bandwidth of an analogue channel used to carry the signal will affect only the horizontal resolution of the image, not the vertical resolution. Excessive curtailment will therefore give an unacceptable image quality, inferior to that which could be obtained with equal horizontal and vertical resolutions.
The present invention is defined by the appended claims to which reference should now be made.
The invention is applicable to both analogue and digital scans. In the former case the image is scanned along a trace formed by a defined co-ordinate sequence, and in the latter case the pixels of the image are scanned in that co-ordinate sequence.
We have appreciated that it would be possible to have a scanning format which is not committed to a line standard and therefore is open to evolution, i.e., the image scanning may be upgraded in acuity without needing a change in the structure of the display. This means that it is downwards compatible. Moreover, it is possible for such a format to be upwards compatible such that the display can be upgraded without changing the source scanning format. Such a technique relies on the use of FRACTALS for defining the scanning locus.
Fractals may be described as structures whose length is undefinable or infinite as the finer the scale used to observe the structure, the greater the apparent length. An example of such a structure is a coastline. The closer it is observed, the greater its length becomes as finer detail becomes resolved.
Such self-similar shapes are neither one- nor two-dimensional shapes as they are defined by conventional Euclidian geometry. That is, they have a fractional dimension.
Fractals may be identical on each level or scale, or may be irregular. A coastline is an irregular fractal. FIG. 4 shows how a regular fractal may be generated. This example is the well known Koch curve or Koch snowflake. The straight sides of an equilateral triangle FIG. 4b (the initiator shown in FIG. 4a ) are operated on by a generator shown in FIG. 4a . This operation produces the result shown in FIG. 4c. The operator is then applied to each of the sides of the shape of FIG. 4c and then subsequently to the sides of the resultant figure, and so on. The result is a figure resembling a snowflake.
It can be shown that the fractal dimension can be defined as
D=-log (N)/log (1/r)
where N is the number of parts of the objected generated and 1/r is the similarity ratio which is used to divide the initiator. For the Koch curve of FIG. 4; N=4 and 1/r=1/3
so that D=1.26
A fuller description of fractals can be found in the book: Mandlebrot FRACTALS--Form, Chance and Dimension, W.H. Freeman, ISBN 0-7167-0473-0. The use of fractals in the field of computer graphics to simulate texture is well established. The use of a fractal curve to explore a multi-dimensional space is known from Stevens, R. J., Lehar, A. F. and Preston, F. H. 1982, "Data ordering and compression of multi-spectral images using the Peano scan", International Conference on electronic image processing July 26-28 1982, IEE conference publication No. 214 pages 209-213. However, the use of a fractal curve to scan an image for transmission and display, with its attendant advantages is thought to be novel.
The invention will be disclosed in terms of a particular fractal--The Peano curve, named after the Italian mathematician Giuseppe Peano, see "Selected works of Guiseppe Peano" translated and edited by Hubert C. Kennedy, ISBN 0-04-164002-0, Allen and Unwin. It is also called Hilbert curve. However, other forms of fractal may be more suitable, in particular the Sierpinski curve, described by Writh, N. in "Algorithms+data structures=programs", Prentice-Hall Inc., ISBN 0-13-022418-9 pages 134-137. In general, the curve may be multi-dimensional; only the two dimensional form is discussed in detail here.
The invention will be described by way of example with reference to the drawings, in which:
FIG. 1 (referred to above) illustrates the sawtooth waveform of conventional raster scanning;
FIG. 2 (referred to above) shows the waveforms required for boustrophedonic scanning in (a) the horizontal (b) the vertical directions;
FIG. 3 (referred to above) illustrates the permissible nonlinearity of the horizontal scan in boustrophedonic scanning;
FIG. 4 (referred to above) illustrates the steps in generating a Koch curve;
FIG. 5 illustrates a fifth-order (32×32) Peano curve;
FIG. 6 illustrates a first-order (basic) Peano curve;
FIG. 7 illustrates a second-order Peano curve;
FIG. 8 illustrates a third-order Peano curve;
FIG. 9 shows the smoothed third-order curve resulting from band-limiting
the coordinate waveforms fairly sharp to half the pixel frequency;
FIG. 10 illustrates a portion of the horizontal and vertical waveforms interpolated by a raised cosine filter;
FIG. 11 illustrates the effect of four-fold averaging and interpolation (filtering) of the scan;
FIG. 12 illustrates the effect of two-fold averaging of the scan;
FIG. 13 illustrates the effect of three-fold averaging of the scan;
FIG. 14 illustrates the effect of 16-fold averaging of the scan;
FIG. 15 illustrates the superposition of the third and fourth-order scans;
FIG. 16 shows the starting and finishing points for various aspect ratios: (a) 2:1 (b) 3:1 (c) 4:1 (d) 3:2 (e) 4:3;
FIG. 17 is a block diagram of a television system embodying the invention;
FIG. 18 is a block diagram illustrating conversion for compatibility with the current technology; and
FIG. 19 is a block diagram of a basic current for generating an n-th order scan.
FIG. 5 shows a two-dimensional fifth-order Peano curve, i.e., a curve connecting an array of 32×32 points. Close inspection shows that it can be divided into quarters, each of which is connected by a single step. The quarters, in turn, can be further subdivided into quarters, again connected by only a single step, and so on. Further, the quarters are seen to be replicas, either directly or rotated through a right angle.
FIGS. 6, 7 and 8 show the first, second and third order curves respectively. It can be seen that each order is derived from the previous order according to simple geometrical rules. Alternatively, the derivation of each order can be considered by way of the Cartesian coordinate sequences as shown in the Appendix below. These sequences, when interpolated, are the waveforms that would need to be applied to the horizontal and vertical deflection circuits of a conventional camera tube or CRT display. Alternatively, they are the horizontal and vertical addressing sequences that would be needed for a discrete display device. The derivation process can be repeated indefinitely to yield higher and higher order curves connecting more and more points.
The Peano scan has three important properties relevant to scanned images:
1. It gives a means of simultaneously altering the horizontal and vertical resolution of the image.
2. The set of curves for different orders form a hierarchical family capable of resolving finer and finer detail.
3. The curves for a particular order `gracefully degrades` to the previous order when smoothed.
The first property arises because the signal obtained by scanning has information in the horizontal and vertical directions in alternating or near alternating fashion. As a result, if the bandwidth of the signal is limited by a bearer channel the resolution of the image is limited equally in both directions. This is the optimum way of using the available bandwidth.
The second property arises because each order is derived from the previous one and so creates compatibility. Taking a running average of four coordinate values and then selecting every fourth average produces the coordinate values of the previous order.
The third property is relevant only to continuous scanning devices such as those using electron beams. The curves in FIGS. 5 to 8 are idealised in the sense that, if the continuously moving scanning spot traces the curve at a constant speed, the x and y coordinate waveforms would be band-limited which would, in general, smooth the corners of the scan. FIG. 9 shows the effect of limiting the bandwidth of the waveforms using a particular filter characteristic which cuts at half the pixel frequency, that is the frequency at which x,y point co-ordinates are generated. This operation would be carried out by the filters following the digital-to-analogue converters generating the waveforms from the coordinate sequences.
There is, however one special case where limiting the bandwidth of the waveforms does not smooth the curve. This is the case of a simple raised-cosine filter pulse response, the base width of the pulse being the pixel spacing. FIG. 10 shows a portion of the waveforms when so filtered. As can be seen, at the ideal point values, each coordinate has zero rate of change and neither overshoots. This means that the spot comes momentarily to rest and, as only one coordinate changes at any time, the motion passes smoothly from one coordinate to the other.
FIG. 11 shows the result of smoothing the scan by taking a running average of four coordinate values and filtering with the first filter. As can be seen, the scan closely resembles that of the previous order except for slight overshoots. FIGS. 12 and 13 show the intermediate situations of two- and three-fold averaging and these clearly show how the scan gradually changes from one order to the next. The two-fold averager appears to join half the number of points, corresponding to a step of half an order. To obtain the next lowest order, appearing to join one sixteenth of the number of points, a 16-fold averaging is necessary, shown in FIG. 14. This again closely resembles the ideal curve. Likewise, an eight-fold averager appears like the two-fold averager of FIG. 12 but one order lower. Averaging by any amount in between corresponds to a curve with intermediate detail. As averaging is a form of low-pass filtering this means that gradually reducing the bandwidth of the coordinate functions causes the curve to gradually change from one order to the next, always retaining its fractal nature.
Given that either the video signal or the scan waveforms may be band-limited to an arbitrary degree, three cases arise at the display. These are:
1. The video and scan bandwidths are equal.
2. The video bandwidth is less than the scan bandwidth.
3. The video bandwidth is greater than the scan bandwidth.
The first case is straightforward in that there are as many independent video samples as there are points in the scan so that each point contributes maximally to the resolution. In the second case the video signal is not changing as fast as it can from point to point and so the resolution is limited by the signal. In the third case the source scan is assumed to be of a higher order than the display. In this case the display will average out of the signal by superposition, either exactly, if discrete, or approximately, if continuous. This can be appreciated by considering adjacent orders of scan. FIG. 15 shows the superposition of third and fourth-order scans. As can be seen, the higher order scan is never more than half a pixel displaced from the lower order. Thus, four adjacent samples of a signal derived on the higher order, if displayed by a continuous scan on the lower order, will suffer no more than half a pixel displacement and so will tend to superpose.
This compatibility between different situations carries the important implication that it is not necessary to know the order of the scan in order to reproduce a version of the image. Thus we have an image transmission system which is independent of the number of pixels in the image. Only the number of fields per second, the form of the fractal (i.e., that it is a Peano curve) and the starting and finishing points need to be standardised.
Thus we have a hierarchical family of scanning standards for transmitting and displaying images such that an image scanned by one member of the family may be displayed by another member of the family without knowledge of the first member. Such an arrangement allows an evolution of scanning acuity to occur.
An apparent theoretical objection to the idea is that it can be applied only to square arrays of points. Arbitrary image aspect ratios are not possible. However, ratios of 2:1 3:1 4:1 3:2 and 4:3 are possible by starting and finishing at the points shown in Figure 16. Small deviations from these values are possible by altering the pixel aspect ratio without departing significantly from the spirit of isotropic resolution.
Because the scan is contiguous there is no flyback except between fields and thus time is saved. Even field flybacks may be eliminated by using a modified square scan consisting of two 2:1 scans joined at their endpoints. Alternatively, a Sierpinski curve may be used which has an inherently endless form. In such a case, synchronising information would have to be sparse, compared with the present systems, possibly consisting of a recognisable framing pattern.
The system is particularly suitable for use with imaging and display devices which are based on discrete rather than continuous scanning. These include systems comprising cameras based on charge-coupled devices (CCDs) for example. Addressable display devices would be particularly suitable.
An outline block diagram of a television system embodying the invention is shown in FIG. 17. Synchronised cameras operating with various orders of scan may be selected at will and their signals transmitted through the channel. The ninth-order scan camera represents, approximately, the current system. The eighth order scan camera represents, say, a low-resolution lightweight `electronic journalism` camera whilst the 10th-order scan camera represents a high definition camera. They could be used in different programmes or even in the same programme. The 11th-order scan camera represents a camera which could be developed in the future, being introduced when required. The same remarks apply to the hierarchy of displays, the eighth-order display representing, say, a wrist-watch receiver based on a liquid crystal display.
The system is capable of being introduced piecemeal and so thus coexisting with current scanning technology. If it were introduced on the channel then compatibility with current technology would require raster-to-Peano converters in conventional cameras and Peano-to-Raster converters in conventional displays, as shown in FIG. 18, the converters merely re-ordering the sequence of incoming pixel values. Such converters would consist simply of a picture store which would write the pixel data in one sequence and read it in another. This re-ordering of data could also be regarded as a scrambling technique to prevent unauthorised reception of a newly-introduced service.
The scan could be generated using a memory addressed by a counter as shown in FIG. 19. An nth order scan would require a memory of 22n locations, each of 2n bits, containing n-bit x and y values and a 2n-bit memory counter able to count from 0 to 22n -1. The contents of the memory could be derived according to the method described in the appendix below. The two outputs of the memory can be used directly to address a discrete scanning device. However, for a continuous scanning device the memory outputs need to be fed to two n-bit digital-to-analogue converters to produce continuous wave forms.
The x and y coordinate sequences for the first order case of Figure 6 are shown in Table 1, in units of the scan step. The y sequence is a palindrome and the x sequence is a complementary palindrome. The coordinate sequences of the second-order case, written in binary form, are shown in Table 2. As there are 4×4 points, each coordinate requires 2 bits and there are 16 entries. The more significant bit is seen to be a replication of the corresponding first-order pattern, each entry being replicated four times. The less significant bit is seen to be the sequence yxxy for the x coordinate or yxxy for the y coordinate where X and Y are the first-order patterns of the x and y coordinates. The first of these sequences is a complementary palindrome and the second is a palindrome.
TABLE 1______________________________________ x y______________________________________ 0 0 0 1 1 1 1 0______________________________________
TABLE 2______________________________________x y x y______________________________________00 00 10 1001 00 10 1101 01 11 1100 01 11 1000 10 11 0100 11 10 0101 11 10 0001 10 11 00______________________________________
TABLE 3______________________________________x y x y x y x y______________________________________000 000 000 100 100 100 111 011000 001 001 100 101 100 111 010001 001 001 101 101 101 110 010001 000 000 101 100 101 110 011010 000 000 110 100 110 101 011011 000 000 111 100 111 100 011011 001 001 111 101 111 100 010010 001 001 110 101 110 101 010010 010 010 110 110 110 101 001011 010 010 111 110 111 100 001011 011 011 111 111 111 100 000010 011 011 110 111 110 101 000001 011 011 101 111 101 110 000001 010 010 101 110 101 110 001000 010 010 100 110 100 111 001000 011 011 100 111 100 111 000______________________________________
Development of the higher order cases proceeds along the same rules. The third-order case, shown in Table 3, has 64 entries of three bit values, the sequences of the first two bits of x and y being the same as those of the corresponding second-order case, each entry being replicated four times. The least significant bit of the x coordinate has the sequence XYYX YXXY YXXY XYYX where X and Y represent the same sequences as before. It can be seen that the initial sequence of each group of four follows the same pattern as the sequences in the first group. Likewise, the least significant bit of the y coordinate has the sequence YXXY XYYX XYYX YXXY. It will be noted that the least significant bits are appropriately palindromic or complementary palindromic.
The rule for derivation of the higher order cases is therefore.
1. The sequence of all but the least significant bit are those of the previous order, each entry being replicated four times.
2. The sequence of the least significant bit consists of groups of four sub-sequences, each taking the form ABBA.
3. The first sub-sequence of the nth group of four is the same as the nth sub-sequence.
4. A can be X or Y or X or Y. If A is X then B is Y and vice versa.
5. The first sub-sequence of x is X if the order is odd and Y if it is even, and vice versa for y.
6. X and Y are the x and y sequences of the first order case.
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|Clasificación de EE.UU.||348/441, 345/25, 365/23, 345/428, 348/325, 348/E03.051|
|Clasificación internacional||H04N7/01, H04N3/30|
|11 Ene 1988||AS||Assignment|
Owner name: BRITISH BROADCASTING CORPORATION, BROADCASTING HOU
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST.;ASSIGNOR:DREWERY, JOHN O.;REEL/FRAME:004818/0342
Effective date: 19871023
Owner name: BRITISH BROADCASTING CORPORATION,UNITED KINGDOM
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNOR:DREWERY, JOHN O.;REEL/FRAME:004818/0342
Effective date: 19871023
|9 Oct 1992||FPAY||Fee payment|
Year of fee payment: 4
|27 Oct 1992||RR||Request for reexamination filed|
Effective date: 19920928
|21 Dic 1993||B1||Reexamination certificate first reexamination|
|4 Feb 1997||REMI||Maintenance fee reminder mailed|
|29 Jun 1997||LAPS||Lapse for failure to pay maintenance fees|
|9 Sep 1997||FP||Expired due to failure to pay maintenance fee|
Effective date: 19970702